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WO2007000766A2 - Procede non invasif permettant d'identifier des corps etrangers dissimules a proximite d'un sujet humain - Google Patents

Procede non invasif permettant d'identifier des corps etrangers dissimules a proximite d'un sujet humain Download PDF

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Publication number
WO2007000766A2
WO2007000766A2 PCT/IL2006/000749 IL2006000749W WO2007000766A2 WO 2007000766 A2 WO2007000766 A2 WO 2007000766A2 IL 2006000749 W IL2006000749 W IL 2006000749W WO 2007000766 A2 WO2007000766 A2 WO 2007000766A2
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WO
WIPO (PCT)
Prior art keywords
radiation
foreign object
frequency band
contrast
signal
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Ceased
Application number
PCT/IL2006/000749
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English (en)
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WO2007000766A3 (fr
Inventor
Yafim Smoliak
Yaakov Lubchik
Nathan Blaunshtein
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
PASSIVE MEDICAL SYSTEMS ENGINEERING Ltd
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PASSIVE MEDICAL SYSTEMS ENGINEERING Ltd
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Publication of WO2007000766A2 publication Critical patent/WO2007000766A2/fr
Publication of WO2007000766A3 publication Critical patent/WO2007000766A3/fr
Anticipated expiration legal-status Critical
Ceased legal-status Critical Current

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Classifications

    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
    • G01J5/0022—Radiation pyrometry, e.g. infrared or optical thermometry for sensing the radiation of moving bodies
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
    • G01J5/0022—Radiation pyrometry, e.g. infrared or optical thermometry for sensing the radiation of moving bodies
    • G01J5/0025—Living bodies
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
    • G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
    • G01N21/35—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
    • G01N21/3581—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light using far infrared light; using Terahertz radiation
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V9/00—Prospecting or detecting by methods not provided for in groups G01V1/00 - G01V8/00
    • G01V9/005—Prospecting or detecting by methods not provided for in groups G01V1/00 - G01V8/00 by thermal methods, e.g. after generation of heat by chemical reactions
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N33/00—Investigating or analysing materials by specific methods not covered by groups G01N1/00 - G01N31/00
    • G01N33/22—Fuels; Explosives

Definitions

  • the present invention relates to a method and device to non-invasively identify hidden foreign objects in proximity of living tissue and more specifically to a method and device that to detect and identify foreign objects hidden under the clothes of a person by measuring an infrared radiation signal emitted by the human subject and by measuring a change in the radiation signal caused by the presence of the foreign object.
  • the present invention is in the class of methods for structural analysis of multi-component materials.
  • the particular multi-component structures/materials of interest include the following components: a human body (living tissue), clothes, and a foreign object that is composed one or more materials and may include metal, magnetic materials, conductive materials or dielectric materials.
  • the object is positively identified based on the interaction of optical radiation naturally emitted by the human body in the infrared frequency spectrum with every component of the examined object.
  • magnetic metal detection and reflected light in the infrared (IR), Ultraviolet (UV) or visible spectrums may be employed to supplement identification based on the IR regime.
  • a living person emits radiation on a wide band of wavelengths. For example, due to its elevated temperature, a human body emits black body radiation in the infrared spectrum. Also the human body reflects radiation in different wavelengths to different degrees.
  • the object affects the radiation field around the person.
  • the present invention detects the presence of foreign objects in proximity to the person including objects hidden behind clothing. Based on the location (including position, as well as shape and size [geometry] of the object) and based on the frequency dependent signature of the radiation anomaly caused by the object, the present invention identifies the foreign object.
  • Detectors are used to identify and exclude dangerous objects from high security zones (for example the boarding areas of civilian aircraft). Also customs, and drug enforcement agencies use detectors to identify foreign substances hidden in or around the body of a person.
  • detectors are metal detectors and x-ray scanners. X-ray and microwave (penetrating radar) scanners are capable of giving high-resolution pictures of hidden objects. The pictures can be used to positively identify dangerous objects and benign objects.
  • x-rays and microwave radiation have the drawback that they are active methodologies requiring exposing objects to high-energy beams of x-ray or microwave radiation. These x-ray and microwave beams are dangerous to people and cannot be used for scanning objects on or near living humans.
  • Metal detectors are safe for use in the vicinity of humans but suffer from two drawbacks.
  • First metal detectors only identify one particular class of dangerous object (those made of metal) but cannot identify other dangerous objects (such as organic explosives, plastic or ceramic weapons, various toxic substances or biological agents).
  • metal detectors are non-specific and cannot differentiate between weapons and benign metal objects of common occurrence (e.g. coins, surgical implants, keys, electronic devices, buttons, zippers). Therefore, where metal detectors are used, a (sometimes lengthy) secondary screening is necessary to preclude non-metallic threats and to determine the nature of detected metal objects. Secondary screening may require intrusive methods such as opening and searching personal baggage, removal of shoes hats or religious apparel and even in some cases strip searches. Such intrusive methods are time consuming, inconvenient, may lead to conflict between security personnel and the public. Reliable routine security systems based on such methodologies are extremely expensive and problem prone.
  • IR radiation infrared
  • Current technologies are based on the integral method of IR-thermal analysis.
  • the integral method consists of the following steps: 1) Measure of the space distribution of the integral heat flow from the object most often from the open surface of the body.
  • thermograph devices and systems e.g. thermo vision [FLIR], thermal cameras, thermographs, radiometers
  • FLIR thermo vision
  • the aim of this method is the structural analysis of the spatial distribution of the flows (usually from narrow bands of IR radiation within the range of 5 ⁇ m - 14//m) from the object and mapping the values of thermodynamic temperature of the structure surface.
  • the integral method of IR - thermograph analysis may also be used for detecting the presence of foreign objects (metallic or non-metallic) hidden inside clothes by measuring an anomaly of the heat flow.
  • Previous art integral methodologies e.g. thermal imaging
  • a homogeneous surface having surface temperature gradient can give a signal like that of a foreign object.
  • the present invention solves the above limitations because the present invention detects the presence of anomalies in radiation over a wide frequency band. Thus, even when some radiation bands are blocked by clothing or masked by temperature differentials, the signature of the foreign object on the remaining bands will be detected. Furthermore, the present invention teaches measuring radiation using a differential measure of radiation intensity.
  • a differential measure for example intensity contrast
  • An absolute measure for example heat flow
  • the use of a differential measure of radiation intensity (e.g. contrast in radiation intensity) makes the present invention more sensitive to subtle anomalies in radiation than previous art methodologies based on absolute measures of radiation intensity (e.g. thermal imaging using a FLIR or a thermal camera).
  • the advantages of using contrast to detect anomalies in radiation is set forth in A.
  • the present invention provides reliable way of detecting, revealing the exact location, the size and form, and identifying the substance of a foreign object hidden under clothes on a human body. This then aids security personal guaranteeing security of transport, sensitive structures or individuals. It also aids in industrial or military security, criminal investigations, control of illegal substances, and custom control of import and export.
  • the present invention is a method and device to non-invasively detect and identify a hidden foreign object in proximity of living tissue. More particularly, the present invention is a method and device to detect and identify a foreign object hidden under the clothes of a human subject by measuring an infrared radiation signal emitted by the subject and by measuring a change in the radiation signal, which is caused by the presence of the foreign object.
  • a method for identifying a foreign object in proximity to living tissue includes the step of finding a location of an anomaly caused by the foreign object in a radiation emitted by the living tissue.
  • the method further includes the steps of performing a spectral analysis of a signal emanated from the location of the anomaly, and identifying the foreign object based on the location and the results of the spectral analysis.
  • a detector for identifying a foreign object in proximity to living tissue.
  • the detector includes a first sensor assembly sensitive to a first frequency band.
  • the first sensor assembly is configured to find a location of an anomaly in a radiation emitted by the living tissue and to enumerate a characteristic of the anomaly.
  • the foreign object causes the anomaly.
  • the detector also includes a second sensor assembly configured to be sensitive to a second frequency band and a processor configured to identify the foreign object. Identification of the foreign object by the processor is based on the location of the anomaly the characteristic of the anomaly and a difference between an unmodified radiation signal emitted by the human tissue and a second radiation signal scanned at the location of the anomaly.
  • Both the unmodified signal and the second signal are in the second frequency band and both signals are detected by the second sensor assembly.
  • the unmodified signal is the radiation signal emitted by the living tissue and unmodified by the foreign object and the second signal is modified by the foreign object.
  • the anomaly is found in radiation including energy in the infrared frequency band.
  • the first frequency band of the radiation includes a wide range of wavelengths spanning from a minimum wavelength of less than 5//m till a maximum wavelength of greater than 12//m.
  • the anomaly is found in a frequency band of the radiation including energy in a first infrared frequency band in the near infrared spectrum of wavelength less than 5//m and also including energy in a second frequency band in the medium infrared spectrum of wavelength greater than 12/rni.
  • the method of identifying a foreign object further includes the step of calculating a differential measure to quantify radiation at the current position of scanning.
  • the radiation is characterized by a differential measure that quantifies the difference between a background radiation and a radiation at the current position being scanned.
  • the differential measure that quantifies radiation at the current position of scanning is a contrast.
  • the method of identifying a foreign object further includes the steps of classifying the foreign object to a general category based on a characteristic of the anomaly in the radiation field, and adapting the spectral analysis to distinguish amongst objects in the general category.
  • the foreign object is given a preliminary classification according to a characteristic of the radiation anomaly caused by the object. The characteristic is a contrast between the a radiation measured at the location of the foreign object and an unmodified radiation emitted by the living tissue without the foreign object
  • the preliminary classification of the foreign object is according to the sign and magnitude of the contrast between the radiation measured at the location of the object and a background radiation level.
  • the foreign object is identified based on a spectral scan made at the location of the object.
  • the spectral scan is adapted to the preliminary classification of the object by choosing a frequency band for the spectral analysis, which is optimal to distinguish between at least two objects in the preliminary general category.
  • the radiation anomaly is detected in a first frequency band and the spectral analysis is performed in a second frequency band.
  • the second frequency band differs from the first frequency band.
  • a background signal emanated by the living tissue without the foreign object is measured in the second frequency band.
  • the location of the anomaly is scanned in the second frequency band resulting in a second measured signal and a contrast is calculated between the first signal and the second signal.
  • spectral analysis is performed on a signal that includes at least one emanation selected from the group consisting of the radiation anomaly resulting from radiation emitted by the living tissue being modified by the foreign object; an output of an external radiation source that interacts with the foreign object; a heat flow from the living tissue; a heat flow from the foreign object.
  • the detector identifies the foreign object based on a difference between an unmodified radiation signal from the living tissue without the foreign object and the radiation signal at the location of the foreign object and the difference is quantified as a contrast between the unmodified radiation signal and the second radiation signal at the location of the foreign object.
  • the first sensor assembly of the detector of the present invention includes an electronic sensor and the second sensor assembly includes the same electronic sensor and a band pass filter.
  • the processing unit of the detector of the present invention is either a human operator or a dedicated electronic processor of a personal computer.
  • Figure 1 is an IR spectrograph of radiation emitted by a human body
  • Figure 2 is a depiction of the physical model that is a basis of the present invention
  • Figure 3 is a first illustration of the results of an integral scan across the chest of a subject using the methodology of the current invention to detect tablet sized object the subject's shirt pocket;
  • Figure 4 is a second illustration of the results of an integral scan across the chest of a subject using the methodology of the current invention to detect a tablet sized object in the subject's shirt pocket;
  • Figure 8 shows the measured transparency coefficient versus the IR wavelength for PM 3 Table
  • Figure 11 shows the measured transparency coefficient versus the IR wavelength for PM 9 Table 6;
  • Figure 12 shows the measured transparency coefficient versus the IR wavelength for PM 10
  • Figure 13 is a flowchart illustrating a method of identifying a foreign object in the vicinity of a living body according to the current invention
  • Figure 14 is a drawing of a first embodiment of the current invention, the embodiment being a handheld device having a single pyroelectric sensor
  • Figure 15 is a drawing of a second embodiment of the invention, the embodiment being a handheld device having a multiple pyroelectric sensors
  • Figure 16 is a drawing of a third embodiment of the invention, the embodiment including a full body scanner with computer controlled graphical interface.
  • FIG. 2 A general illustration of the physical model (PM) that is the basis of the present invention is presented in Figure 2.
  • a foreign object 8 is identified based on interactions between foreign object 8 and infrared radiation emitted by the human body 10.
  • the presence of clothes 6 or foreign object 8 causes changes in the IR radiation field.
  • the nature of these changes in the radiation field is depends on the transparency, reflectance and transmittance of clothes 6 and foreign object 8.
  • the transparency, reflectance and transmittance of clothes 6 and foreign object 8 are dependent on the substance, geometry and temperature of clothes 6 and foreign object 8.
  • Clothes 6 and foreign object 8 display different transparency, reflectance and transmittance for different wavelengths of the IR radiation band.
  • the intensity of radiation in a given wave band that is emanated by a composite object (as in Figure 2) wherein a black body heat emitter (human body 10) is obscured by one or more objects (e.g. a foreign object 8, and clothes 6) can be computed using the formulas shown in Table 1 and parameters from
  • the PM of the current invention includes the following basic components (see Figure 2):
  • Radiator - is human body 10, which behaves as a blackbody at temperature T R .
  • Foreign Object 8 - is a selectively emitting body (metal, plastic, etc.) at temperature T F0 .
  • Clothes 6 - is treated as a gray-body at temperature T Q .
  • the optical parameters that are used in the proposed physical model are: Radiator - the spectral density of emitted radiation (dR/d ⁇ ) from human body 10 as a black body with temperature T R (for Radiator), which is assumed to be nearly identical to radiation emitted by an ideal black body heated to the temperature of a human body.
  • Foreign Object 8 - the spectral coefficients of emissivity, ⁇ ( ⁇ ), transparence, ⁇ ( ⁇ ), and reflectance, 7-( ⁇ ) for Foreign object 8; and
  • Clothes 6 - integral coefficients of emissivity, ⁇ ; transparence, ⁇ ; and reflectance, r for Clothe 6. Parameters of the model are presented in
  • Scanning was performed by means of a scanning mirror system. Alternatively scanning is done using a mechanical entrance aperture with changeable entrance hole value or by moving the detector (e.g. investigator waving a hand held detector). The scanning of the investigated structure surface allows marking the outline of the foreign object 8, hidden in the clothes 6 on the human body 10.
  • preliminary classification of a foreign object is based on the absolute value of the contrast and the sign of the contrast during the integral scan. For example based on the experimental integral flow measurements, whose data is presented in Table 4 and Table 5, on the overall magnitude (in %) and sign of the contrast for different foreign objects and materials, the first classification of the detected foreign object can be made.
  • positive contrast values of greater than 50% are received only from objects from steel or from objects containing iron, like an electron device having electron elements in a plastic case. Therefore objects producing positive contrast of greater than 70% are identified to have metallic elements of more than 5 mm thickness. Contrast magnitudes of 20% and up to 30% are found for both plastic and explosive materials (e.g. TNT).
  • the final identification is made according all received results from integral and narrow band passive measurements. This identification is based on choosing the most suitable substances and objects, wliich have properties similar to those measured. Alternatively, in cases where a more precise identification is needed or where there is a need to detect small quantities of specific materials (for example biological or nuclear materials) the passive IR (integral and spectral regimes may be supplemented by a Geiger counter, a metal detector or an active optical regime (such as irradiating the subject with a low power IR or UV bulb and measuring reflected light).
  • the passive IR integrated and spectral regimes may be supplemented by a Geiger counter, a metal detector or an active optical regime (such as irradiating the subject with a low power IR or UV bulb and measuring reflected light).
  • a subject 1 (a man passing a security check) is a man wearing clothes 6 and carrying a foreign object 8.
  • the current invention takes advantage of the fact that when the infrared optical field, radiated from body 10 of the subject is influenced by a foreign metallic or dielectric foreign object 8, even if foreign object 8 is hidden or embedded into clothes 6, the difference between the temperature between foreign object 8, human body 10 and the clothes 6 leads to an anomaly in the radiation field emitted by human body 10.
  • a detector 2 detects the anomaly in the radiation field. Detector 2 scans by moving in a direction 4. Li Figure 2, detector 2 has yet to reach foreign object 8.
  • detector 2 is beyond the boundary of foreign object 8, and detector 2 detects the background radiation emitted by human body 10 and attenuated by interposing clothes 6.
  • detector 2 scans (moving in direction 4)
  • detector 2 will pass over a leading edge 5a of the foreign object 8.
  • the detected radiation will jump to the anomalous radiation emitted by human body 10 and attenuated both by clothes 6 and by foreign object 8.
  • the radiation field jumps again from the anomalous level back to the background level.
  • the anomaly in the radiation field is detected.
  • the background radiation field is detected.
  • the locations of leading edge 5a and trailing edge 5b and therefore the location and geometry in one dimension of foreign object 8 are known. Scanning in various directions and using known tomographic methodologies, the 3-dimensional position of foreign object 8 is measured.
  • FIG 13 a flow chart of a first embodiment of the present invention.
  • a security guard is using the scanning device of Figure 14 to test for a foreign objects.
  • the guard measures 13 the integral background radiation level (unmodified by the presence of foreign object 8).
  • a human operator using a hand held instrument 100 measures 13 an integral background radiation level and calibrates for an integral scan 12 by holding the sensor 108 over a part of subject 1, where there is no hidden object and where the radiation emitted by subject 1 is substantially unmodified by foreign object 8.
  • Sensor 108 is a pyroelectric detector.
  • the pyroelectric detector is sensitive to IR radiation in the bandwidth from 5 ⁇ m — 20 ⁇ m.
  • integral scan 12 measures the average radiation intensity in this wide bandwidth.
  • the operator To measure 13 the background radiation level and calibrate the instrument, the operator first puts instrument 100 into a integral-background mode by first pressing integral-scan-button 102a and then pressing background-toggle-button 102d. Once in the integral-background mode, the operator starts integral scan 12 by pressing on-button 104e causing instrument 100 to register the mean radiation density (0.0015 W/cm 2 ⁇ m) on gauge 110 and also causing the instrument 100 to calibrates itself by measuring and storing a background radiation level (if there is a foreign object present at this location, the subject will be sent to secondary inspection due to an abnormal background [see step 20 of Figure 13]).
  • an operator measures 13 a background radiation level by calibrating instrument 100 periodically on an airport worker (wearing typical clothes and not having a foreign object), or by manually setting a general expected background radiation intensity level ⁇ 2xlO ⁇ 3 W/(cm 2 ⁇ m) [See Figure I].
  • a photographic filtering method in visual optics waveband is used, (as described in A. T. Nesmyanovich, V. N. Ivchenko, G. P. Milinevsky, "Television system for observation of artificial aurora in the conjugate region during ARAKS experiments", Space Sci. Instrument, vol. 4, 1978, pp. 251-252. and in N. D. Filipp, V. N. Oraevskii, N. Sh. Blaunshtein, and Yu. Ya.
  • the following general steps are performed to detect a foreign object using integral heat contrast: a) measuring of the space distribution of the integral heat flow radiated from the structure in the range of wavelength from 5 ⁇ n — 20//m; b) detecting and outlining of the anomalies of the heat flow, which we defined above as a contrast, radiated from the structure's surface; c) classifying the cause of the detected radiation anomaly (the foreign object) by a characteristic of the integral radiation measurement, for example, the sign and the absolute value of the heat flow changes (i.e., the sign and the magnitude of the contrast).
  • a characteristic of the integral radiation measurement for example, the sign and the absolute value of the heat flow changes (i.e., the sign and the magnitude of the contrast).
  • the contrast of the corresponding foreign structure is also changed, and the resulting contrast can be positive or negative at the optical recorder.
  • the operator finds 16 an anomaly in the radiation field by noticing any jump in the contrast representing the border of foreign object 8.
  • the detection of metallic or dielectric foreign object 8 is made according the level of the resulting contrast.
  • This integral method provides a reliable definition of the location and dimensions of the detected foreign object, because the interaction of the infrared field irradiated from human body 10, as a passive source of infrared radiation with the foreign object is going on not only near the contour of foreign object 8, but at the some distance from it.
  • the current invention uses a wide range of frequencies in the integral regime. Thus, the current invention can detect a wide array of objects hidden behind clothing and even under human skin.
  • Gauge 110 registers the magnitude of contrast between the measured radiation at the current focus of sensor 108 and the measurement of background radiation stored during the calibration step.
  • a threshold 2%
  • an alarm is sounded over loudspeaker 105 to alert the operator that the current location contains a radiation anomaly.
  • the operator enumerates 22 characteristics of the radiation anomaly including the location of the wand when there the jump in contrast occurs and in the contrast at the location of the anomaly in the radiation field.
  • the operator finds 16 no jumps in the measured radiation during the integral scan 12 and then there are no locations of radiation anomalies that need to be scanned. Nevertheless, the operator checks 18 that the background radiation is normal not only in its integral value, but also in narrow spectral bands.
  • the instrument of Figure 14 is capable of measuring three narrow bandwidth portions of the spectrum. The first narrow bandwidth is 5-7 ⁇ m.
  • the operator first depressing button 102b to set the 5 — I ⁇ m band pass filter. Then in order to make a background scan the operator first toggles-on the calibration function by depressing background-toggle-button 102d, and starts measuring the background radiation level by depressing the on-button 102e.
  • button 102c is pressed. Then in order to make a measurement, the background toggle button 102d is depressed, and finally to actually start measuring the background radiation, on-button 102e is depressed. Then the background radiation level registered as a radiation intensity on gauge 110. If the intensity of all of the narrow band measurements is determined 20 to be within a range considered normal, subject 1 passes inspection 60 and is allowed to continue to his destination in the security zone. If one measured background radiation level is not within a normal range, subject 1 is sent to secondary inspection 50.
  • the operator When the operator finds 16 jumps in contrast during integral scan 12, then the operator enumerates 22 the characteristics of the jumps (locations and measured contrast) for each foreign object. The operator then chooses a location where no foreign object was detected and for each spectral band first performs 24 a spectral background measurement (as described above step 18). The result is the spectral background level (i.e. a background energy level for each wavelength [R" (X)]. If a background radiation level in the spectral measurement is determined 26 to be not within a range considered normal, the subject is immediately sent to secondary inspection 50.
  • a background radiation level in the spectral measurement is determined 26 to be not within a range considered normal, the subject is immediately sent to secondary inspection 50.
  • a background radiation level and the results of the spectral measurement is determined 26 to be within a range considered normal 24, then a location of an unidentified object is chosen and the operator identifies 28 the object. Particularly, the operator first preliminarily classifies 30 foreign object 8 according to characteristics of the contrast of the integral measurement. If the contrast is positive and it is greater than 50% 40, then the object is classified as a metal object (according to Table 5 only metal objects have such high positive contrast) and the subject is sent to secondary inspection 50. If there is a positive contrast 30 of less then 50% 40, then the object is classified as either metal, polyester or polyethylene (according to Table 5 all of these substances display high positive contrast).
  • the spectral scan is adapted to differentiate between metal and polyester and polyethylene by choosing a narrow spectral band 10 — 14/an.
  • the 10 — 14/an band is optimal for differentiating these materials because in this band metal displays a positive contrast while plastics display negative contrast as can be seen in Figure 7.
  • the background-toggle-button is depressed (toggling off the background mode) and the location of the object is scanned 42 at 10 — I4jum by holding the sensor over the location of the detected object and depressing on- button 102e. If the contrast is determined 44 to.
  • the 5 — 7//m band is optimal for separating explosives from plastic because at 5 — 7//m, plastic has a positive contrast (as shown for objects 3, 6, and 9 in Figure 5) and explosives have a negative contrast.
  • the location is then scanned 32 in the spectral mode at the 5 — 7/an wavelength band. If the contrast of 5 — I ⁇ m scan 32 is determined 34 to be negative, then subject 1 is identified as suspected of holding a hidden explosive device and is sent to a shielded room for special inspection. If the contrast of 5 — I ⁇ m scan 32 is determined 34 to be positive, then the object of the current location is identified as plastic and if there are not found 38 any other unidentified object, then subject 1 passes inspection 60 and is allowed to go on to his intended destination.
  • the embodiment of Figure 15 includes multiple sensors assemblies 208a, 208b, 208c, and 208d.
  • Each sensor assembly 208a — 208d is configured to perceive radiation in a different bandwidth.
  • sensor assembly 208a is configured to be sensitive to radiation in a wide spectrum from 5 ⁇ x — 20//m;
  • sensor assembly 208b is configured to be sensitive to radiation from 4.5/fln — 5.5//m;
  • sensor assembly 208c is configured to be sensitive to radiation from 13.5//m — 14.5/zm;
  • sensor assembly 208d is configured to be sensitive to radiation from 9.5//m —
  • FIG. 15 of an instrument 200 is supplied with two buttons, and on- button 202a and a background-calibration-button 202b.
  • instrument 200 measures and detects a background radiation level simultaneously with all four sensor assemblies 208a — 208d and stores a background level for each of the four corresponding bandwidths. If the background level in one of the bandwidths is outside of a preset "normal" range, the instrument notifies the operator by sounding an alarm on loudspeaker 105 and displays a message explaining the nature of the abnormal reading (high or low radiation levels in a particular bandwidth) on LCD display 212.
  • instrument 200 When only on-button 202a is depressed, instrument 200 detects radiation levels using all four sensors 208a — 208d each measuring radiation in a corresponding bandwidth. A microprocessor inside of instrument 200 compares the measured radiation level in each bandwidth with the radiation level of the corresponding bandwidth stored during the background-calibration step. Results are displayed on LCD display 112. When a foreign object 8 causes a jump in the contrast of at least one of the bandwidths beyond a threshold value (absolute value of 2%) then the operator is notified by an alarm over speaker 205. Thus, the integral mode of scanning simultaneously detects anomalies in the radiation signal in all four bandwidths.
  • LCD screen 112 presents a message identifying the object. Specifically, identification is based on analysis by the microprocessor of the contrast in the four bandwidths. For example, if all four sensors assemblies (208a — 208d) detect a positive contrast, the LCD displays the message "metal object detected).
  • the LCD displays the message "explosives detected.”
  • the, loudspeaker 105 is deactivated in order to allow evacuation of the area before alerting subject 1 that explosives have been detected. If sensor assembly 208d senses a negative contrast while some of the remaining sensors 208a — 208c register a positive contrast, LCD display 212 displays a message "Plastic object detected”.
  • Figure 16 illustrates a third embodiment of an instrument 300 to detect and identify foreign object 8 according to the present invention.
  • a full body scanner 302 contains sensors configured to scan across a subject 1.
  • Full body scanner 302 may be a simple metal detector, or it may include more sophisticated sensors. If fast conclusive results are important and money is not an object, full body scanner may contain multiple IR sensor assembalies.
  • Full body scan results are sent to a desktop computer 306.
  • Desktop computer 306 conveys an image 308 of subject 1 to a display device 310 (a computer monitor). Also output to the display device 310 is a label 312, showing the state of identification of foreign objects in the vicinity of subject 304. For objects that are not yet fully identified, the operator has a hand scanner instrument 200, which is also integrated to desktop computer 306.
  • computer 306 includes 3D tomography software that tracks the location of instrument 200.
  • information from scanner 200 is automatically added to a database on subject 1 and based on the location and results of the scan, unidentified object label 312 is updated according to the results of a scan using instrument 200.
  • scanner assembly 302 facilitates fast recognition of a large number of foreign objects by an operator. Furthermore, the operator of scanner assembly 302 is located at a distance from subject 1 and therefore is safe from attack or explosions initiated by subject 1. Scanner assembly 302 is further controlled via desktop computer 306. Thus the operator can adjust contrast, image quality, scanning speed, and scanning frequency bandwidth using a keyboard 314. Alternatively, scanner assembly 302 is also equipped with special detectors for example a metal detector, a Geiger counter and an active scanner in the optical or ultraviolet bandwidth to further facilitate positive identification particular substances in smaller quantities than those detectable by IR scanning.
  • special detectors for example a metal detector, a Geiger counter and an active scanner in the optical or ultraviolet bandwidth to further facilitate positive identification particular substances in smaller quantities than those detectable by IR scanning.
  • Table 1 Formula for calculating the contrast —A formula for calculating contrast between radiation flux measured from a human body in the presence a foreign object and radiation flux from a human body in the absence of a foreign object.
  • R 0 ⁇ ) R( ⁇ ) ⁇ [ ⁇ s ( ⁇ )r o ( ⁇ )+ ⁇ o ( ⁇ )] ⁇ c ( ⁇ )+ ⁇ c ( ⁇ ) ⁇ ; (IB)
  • T ⁇ ) [ ⁇ o ( ⁇ ) ⁇ c ( ⁇ )] 100%. (IG) where :
  • R 0 ( ⁇ ) is an emitted radiation flux from the Human Body, when the Foreign Object (FO) (as a component of PM) presents;
  • R c. ( ⁇ ) is an emitted radiation flux from Human Body, when the FO (as a component of PM) is absent;
  • R'( ⁇ ) is an emitted radiation flux from black-body (human skin) in spectral step ⁇ at temperature r R ;
  • ⁇ is (/Imax - /Lmin) / N ; /Lmin ⁇ ⁇ ⁇ Imax ;
  • C( ⁇ ) is a contrast in spectral step ⁇
  • ⁇ 7 ⁇ is a spectral coefficient of optical transparence of emitted radiation from black-body, through the Object and Clothes, at temperature T in spectral step ⁇ .
  • This coefficient (in %) determines the share of radiation penetrated (run) through the PM components;
  • ⁇ s is the heat radiation coefficient of blackness of the human skin;
  • ⁇ o is the heat radiation coefficient of blackness of the foreign object;
  • ⁇ c is the heat radiation coefficient of blackness of the clothes;
  • ⁇ 0 is the transparent coefficient of the foreign object;
  • r c is the transparent coefficient of the clothes.
  • Table 2 Optical properties of the clothes — The optical properties of clothes used in equations predicting the integral heat flux.
  • Table 3 Optical properties of the common substances — The optical properties of common substances used in equations predicting the integral heat flux in the presence of a foreign object.
  • Table 5 Measured contrast in the integral regime — The contrast measured between integral radiation for a dressed human subject in the presence of a foreign object and in the absence of the foreign object for various combinations of clothes and foreign objects.
  • Table 6 Components of PM investigated in spectral regime — A list of physical models (clothes and foreign objects) tested in the spectral regime (results reported in Figure 5 - Figure 12).

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Abstract

L'invention concerne un procédé et un dispositif permettant d'identifier de manière non invasive des corps étrangers dissimulés à proximité de tissus vivants. De manière plus spécifique, l'invention se rapporte à un procédé et à un dispositif permettant de détecter et d'identifier un corps étranger dissimulé sous les vêtements d'une personne par mesure d'un signal de rayonnement infrarouge émis par un sujet humain, et par mesure d'une modification du signal de rayonnement causé par la présence du corps étranger. Ce procédé se classe dans les procédés d'analyse structurelle de matériaux à composants multiples. Les structures/matériaux à composants multiples particuliers recherchés comprennent les composants suivants: corps humain (tissus vivants), vêtements, et un corps étranger composé d'un ou de plusieurs matériaux et pouvant contenir des métaux, des matériaux magnétiques, des matériaux conducteurs, ou des matériaux diélectriques. Ce procédé permet d'identifier positivement le corps étranger même lorsque celui-ci est dissimulé sous les vêtements, à partir de l'interaction du rayonnement optique dans le spectre de fréquences infrarouges émis naturellement par le corps humain avec chaque composant de l'objet examiné.
PCT/IL2006/000749 2005-06-28 2006-06-27 Procede non invasif permettant d'identifier des corps etrangers dissimules a proximite d'un sujet humain Ceased WO2007000766A2 (fr)

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